1. No category

Labunov et al. Nanoscale Research Letters 2013, 8:375
http://www.nanoscalereslett.com/content/8/1/375
NANO EXPRESS
Open Access
Femtosecond laser modification of an array of
vertically aligned carbon nanotubes intercalated
with Fe phase nanoparticles
Vladimir Labunov1†, Alena Prudnikava1*†, Serguei Bushuk2†, Serguei Filatov3†, Boris Shulitski1†, Beng Kang Tay4,
Yury Shaman5 and Alexander Basaev5
Abstract
Femtosecond lasers (FSL) are playing an increasingly important role in materials research, characterization, and
modification. Due to an extremely short pulse width, interactions of FSL irradiation with solid surfaces attract special
interest, and a number of unusual phenomena resulted in the formation of new materials are expected. Here, we
report on a new nanostructure observed after the interaction of FSL irradiation with arrays of vertically aligned
carbon nanotubes (CNTs) intercalated with iron phase catalyst nanoparticles. It was revealed that the FSL laser
ablation transforms the topmost layer of CNT array into iron phase nanospheres (40 to 680 nm in diameter) located
at the tip of the CNT bundles of conical shape. Besides, the smaller nanospheres (10 to 30 nm in diameter) are
found to be beaded at the sides of these bundles. Some of the larger nanospheres are encapsulated into carbon
shells, which sometime are found to contain CNTs. The mechanism of creation of such nanostructures is proposed.
Keywords: Femtosecond laser ablation; Carbon nanotube array; Iron phase nanosphere; Chemical vapor deposition
PACS: 61.48.De, 06.60.Jn, 42.62.Cf
Background
Ultrafast lasers are playing an increasingly significant
role in materials research, characterization, and surface
morphology modification due to a number of unexpected phenomena and formation of new structures. For
the past 10 years, being the leading material in semiconductor and photonic industries, silicon has attracted
majority of interest and the modification of its surface
morphology in different environments using the femtosecond laser (FSL) irradiation has been intensively
studied [1-9].
The initial discovery was made when a polished silicon
surface was transformed into a forest of quasi-ordered
micrometer-sized conical structures upon exposure to
several hundred FSL pulses in an atmosphere containing
sulfur hexafluoride (SF6) [10,11]. These conical structures
* Correspondence: prudnikova@bsuir.by
†
Equal contributors
1
Laboratory of Integrated Micro- and Nanosystems, Belarusian State
University of Informatics and Radioelectronics, P. Brovka St. 6, Minsk 220013,
Republic of Belarus
Full list of author information is available at the end of the article
could trap a large quantity of sulfur doping the semiconductor at a concentration that was well above the solubility limit. The confluence of these chemical and structural
changes has yielded a unique new material with novel optical properties that have never been observed. This material absorbed about twice as much of visible light as
compared to normal silicon and had the ability to detect
infrared light that is invisible to the current generation of
silicon detectors; also, it possessed significant advantages
in detection, imaging, and power generation applications
[3,9,12-14]. Lately, various morphology and property
changes were reported that have resulted from the FSL irradiation with different varieties of ambient, including
various gaseous, as well as vacuum, liquid, water, and air
[2,5,6,15-17].
Over the past two decades, carbon nanotubes (CNTs)
have attracted a lot of attention due to their exceptional
properties [18,19], and as it is expected, potentially, they
can replace silicon in the emerging nanoelectronics and
nanophotonics.
Hence, investigating the interaction of FSL irradiation
with CNTs would represent a great interest. The first
© 2013 Labunov et al.; licensee Springer. This is an Open Access article distributed under the terms of the Creative Commons
Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction
in any medium, provided the original work is properly cited.
Labunov et al. Nanoscale Research Letters 2013, 8:375
http://www.nanoscalereslett.com/content/8/1/375
result that is useful for our investigation was obtained
while studying the light interaction with fluffy arrays of
single and multiwall CNTs containing metal (Fe) catalyst
nanoparticles using a photoflash [20-24]. Photoacoustics
and ignition have been observed in these arrays. The
mechanism of ignition was attributed to the light absorption by CNT arrays due to the black body effect that generated rapid increase in temperature. As a result, a chain
oxidation reaction of CNTs and metal nanoparticles was
initiated which caused ignition; as a result of which,
nanoparticles containing Fe2O3 and Fe3O4 [24] or C, O, Si,
and Fe [23,24] were produced. The most important result
of this investigation was that the metal nanoparticles are
playing significant role in the deposited energy absorption.
A number of investigations were performed with the
laser irradiation of arrays of dense vertically aligned
CNTs which have been pursuing the aim of pattering
the arrays in order to obtain the configurations of some
devices. This process is known as laser pruning [25],
burning [26], or laser machining [27]. The lowering of
the nanotube density and formation of nanotube junctions and nanoparticles via laser surface treatment were
well reported [25-27]. To our best knowledge, only in
few works, the femtosecond laser pulses were used for
CNT treatment, for example [27,28], while in the rest
continuous irradiation of the gas or solid state lasers was
utilized [25,26,29,30]. What is important is that in all
aforementioned studies, CNT arrays were synthesized by
different chemical vapor deposition (CVD) methods, either thermal, hot filament, or plasma enhanced, but in
all of them, the localized on the substrate catalysts (Fe
or Al/Fe) were used. As a result of this technology
utilization, the CNT arrays did not contain metal catalyst
nanoparticles. This situation determines the interaction
process itself and the obtained products of interaction
and could be considered as the simplest case of the laser
irradiation interaction with the CNT arrays.
In the present work, we investigate for the first time
the interaction of femtosecond laser irradiation with the
arrays of vertically aligned carbon nanotubes intercalated
with the ferromagnetic (Fe phase) nanoparticles. The
presence of metal nanoparticles in CNT array, as it was
shown in [20-23], plays the important role in the energy
absorption by the array. The importance of the present
investigation is defined by the possible applications of
the obtained results. The arrays of CNTs with the intercalated ferromagnetic nanoparticles, so called magnetically functionalized CNTs (MFCNTs) [31,32], may be
considered as an ideal medium for different magnetic
applications. They can be used as sensors, sensitive elements of magnetometers, magnetic filters, ferrofluids,
xerography, magneto-resonance imaging, magnetic hypothermia, and biomedical applications. The superior
application of oriented MFCNT arrays can be in a
Page 2 of 10
sphere of magnetic write/read heads and high-density
data storage devices [33-36]. The FSL irradiation may
become an instrument for the machining of the mentioned devices based on the arrays of MFCNTs.
In particular, in the present work, we investigate the
surface morphology modification of the vertically aligned
MFCNTs upon FSL irradiation and properties of the
products obtained after irradiation and develop the mechanism of the interaction of FSL with such complicated
media as the arrays of MFCNTs.
Methods
CNT arrays were synthesized on Si substrates by the
floating catalyst CVD via a high-temperature pyrolysis of
the xylene/ferrocene solution injected into the reaction
zone of quartz reactor. In our particular case, the concentration of ferrocene in the solution was 10%; the
temperature in the reaction zone was 875°C, and the
process duration was 30 s. Obtained as a result of ferrocene decomposition, Fe phase nanoparticles serve as
catalyst for CNTs growth. During the growth process,
these nanoparticles are intercalating into CNT arrays
and are considered as fillers of CNTs.
The morphology of the CNT arrays before and after the
FSL irradiation was investigated by scanning electron microscopy (SEM) (Hitachi S-4800 FE-SEM, Chiyoda-ku,
Japan). For Raman measurements, Renishaw microRaman Spectrometer (Series1000, Renishaw, Wottonunder-Edge, UK) with laser beam of 1.5 mW incident
power and 514 nm wavelength was used. The structure of
CNTs was characterized by transmission electron microscopy (TEM, JEM 100-CX, JEOL) and a high-resolution
TEM (JEM-2010, JEOL Ltd., Akishima-shi, Japan). For
X-ray diffraction analysis (XRD), DRON-3 diffractometer
(Bourevestnik, Inc., Maloochtinskiy, Russia) was used; the
local configurations of iron ions of CNTs fillers were examined with Mössbauer spectroscopy (spectrometer
MS2000 with Fe/Rh source, 40 mCu). Elemental analysis
was made by energy-dispersive X-ray spectroscopy (EDX)
(SUPRA-55WDS with the EDX prefix, Carl Zeiss, Inc.,
Oberkochen, Germany).
The FSL irradiation was performed in ambient atmosphere with laser scanning microscope (Zeiss LSM 510
NLO based on Zeiss Aviovert 200 M inverted research
microscope). This setup is equipped with femtosecond
titanium-sapphire laser (Spectra-Physics Tsunami, Santa
Clara, CA, USA) delivering 100 fs pulses at a wavelength
of 790 nm with 82 MHz repetition rate. The energy of a
single pulse was 15 nJ. The laser beam was then focused
by Zeiss Plan-Neofluar 40x/0.75 objective and formed a
spot with 1.2 μm in diameter on the sample surface. The
beam was attenuated with an acoustic-optical filter to
the energy level of 6.25nJ per pulse at the focal plane of
the microscope objective. The investigated samples were
Labunov et al. Nanoscale Research Letters 2013, 8:375
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Page 3 of 10
placed onto the stage of the microscope without cover
glass. CNT array treatment was achieved by scanning
line-by-line at 512 lines per scan resolution. The scan
speed was about 145 mm/s. The dimension of the scan
area could be varied from 230 × 230 μm to 30 × 30 μm.
Zoom factor of the microscope was chosen equal or
a
greater to the required Nyquist criterion to ensure the
focal spot overlaps between neighboring lines. Threedimensional scanning is achieved with a built-in Z-axis
drive. The step of Z-axis was chosen to be 1 μm, again
to ensure the spatial overlapping of the focal spot between neighboring planes.
b
1
100 nm
d
c
2
1400
Intensity, a.u.
1200
1000
800
600
400
200
0
0
500
1000
1500
2000
-1
Raman shift, cm
20
10
0
20
inten sity, a .u .
30
0,9990
(313)Fe3C
40
f
(400) Si
(222)Fe3C
50
(021)Fe5C2
(110)Fe
(211)Fe3C
(122)Fe3C
(004)Fe3C
Intensity, a.u.
60
substrate
(112)Fe3C
(201)Fe3C
70
(002) graphite
e
0,9975
experiment
total
FeC2
0,9960
0,9945
γ-Fe
Fe3C
α-Fe
0,9930
30
40
50
2θ
60
70
80
-6
-4
-2
0
2
4
-1
velocity, mm s
Figure 1 Characteristics of the obtained CNT array grown on Si substrate. (a) Morphology (SEM). (b) TEM image of CNTs with the filler in
the CNTs channels (1) and walls (2). (c) HRTEM image of a multiwall CNT with the filler in its channel. (d) Raman spectrum. (e) XRD pattern.
(f) Mössbauer spectrum.
6
Labunov et al. Nanoscale Research Letters 2013, 8:375
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Results
The characteristic morphology and composition of the
obtained CNT array as well as the CNT structure are
depicted in Figure 1a,b,c,d,e,f. Figure 1a shows the SEM
image of the synthesized dense vertically aligned CNT
array. Figure 1b,c shows the TEM images of the synthesized CNTs which are found to be multiwall, with outer
diameters of 12 to 70 nm. From Figure 1b, it is seen that
some CNTs are filled with nanoparticles (1) in the
channels of CNTs and (2) in between their walls.
Figure 1d corresponds to the Raman spectrum collected
from the sample which contains D peak (approximately
1,358 cm−1) arising from the structural disorder and G
peak (approximately 1,584 cm−1) common to all sp2 carbon forms. The ratio of intensities IG/ID = 2.47 testifies
that CNTs are well crystallized and have low defect concentration. The XRD pattern in Figure 1e shows that the
CNT array contains graphite (002) with a rhombohedral
structure [37] (ICDD card no. 75–2078, PCPDFWIN),
which is a characteristic of CNTs. Besides, the XRD pattern exhibits a series of peaks corresponding to Fe phase
(including carbides): Fe3C and Fe5C2. Analysis of the
XRD result reveals that carbide Fe3C with an orthorhombic structure (space group Pbnm) dominates over
the other phases of nanocomposite (approximately 90%)
[32,38]. The Mössbauer spectrum collected in transmission geometry at room temperature is shown in Figure 1f,
and the hyperfine parameters (subspectra) are summarized in Table 1. It has been specified that these states of
iron are fcc γ-Fe, bcc α-Fe, and Fe3C. However, the
spectrum does not reveal the state of Fe5C2 but instead
the doublet of FeC2. This discrepancy can be attributed
to the difference in sensitivity between the two methods.
A SEM image of the FSL irradiated area of CNT array
is presented in Figure 2. The size of the irradiated zone
is 200 × 200 μm2 (Figure 2, inset). It can be observed that
upon the FSL irradiation, a square cavity of approximately
10 μm in depth was created. Nanoparticles of spherical
shape were found at the bottom of the cavity located at
the tips of conical shape CNT bundles. It is more prominent to observe these nanostructures at the walls of the cavity (indicated as ‘1’ in Figure 2). Also, some of these
nanospheres (indicated as ‘2’ in Figure 2) are found to be
sited slightly away from the irradiated area.
Table 1 Hyperfine parameters of the Mössbauer spectrum
shown in Figure 1f
Subspectrum
δ
ΔЕ
Нeff
(mm/s)
(mm/s)
(T)
Singlet С
−0.13
0
-
20
γ-Fe
Doublet D
0.20
0.52
-
13
FeC2
Sextet S1
0.17
0
20.6
54
Fe3C
Sextet S2
−0.06
−0.03
32.6
13
α-Fe
Contribution
Phase
In Figure 3a, the SEM image of the irradiated area is
presented. It is seen that the nanospheres found at the
tips of the CNT bundles (1,2) generally have a larger diameters, while those that are found to be beading the
CNT bundles (3) have the smaller ones (approximately
10 to 30 nm). From Figure 3a, it is clearly seen that
there are two types of larger nanospheres. Some of them
are enveloped by the shells of a very complicated structure (2), whereas others do not have shells (2).
In Figure 3b,c, the quantitative analysis on the size distribution of the nanospheres of type (1, 2) is presented.
It is seen that these nanospheres have a wide radius distribution (20 to 340 nm) with predominant radius in the
range of 30 to 70 nm.
The TEM images are presented in Figure 4a,b,c. In
Figure 4a, it can be seen clearly that some of the
nanospheres are encapsulated within a shell (1), while
some are not (2). Besides, the diameters of CNTs attached to the nanospheres are found to be smaller
(approximately 5 nm), as compared to CNTs before laser
irradiation (Figure 1b). Smaller nanospheres can also be
seen attaching to the outer walls of CNTs (3). Figure 4b
represents big size nanospheres covered by the shell (1),
which contains some inclusions (2) and a number of
easily recognized CNTs (3), whereas in Figure 4c, the
magnified image of the nonencapsulated nanosphere is
shown.
The EDX spectroscopy was employed in order to obtain a general overview of element distribution in the
formed structure (Figure 5a,b,c,d). To have a better understanding within the nanostructure, partial of the
CNT array was removed with a high-intensity FSL beam.
The corresponding EDX image of the investigated area
is shown in Figure 5a. In this figure, dark blue region
corresponds to Si substrate, blue corresponds to CNTs,
and green represents the nanospheres. Figure 5d shows
the EDX spectrum demonstrating signals of Si, O, Fe,
and C.
The in-depth quantitative analysis of the elemental
composition within the nanosphere was obtained with a
localized EDX analysis across its diameter with a 30-nm
diameter electron beam spot. In Figure 5b, ten scanning
spots across a 600-nm diameter nanosphere are depicted
and in Figure 5c, the corresponding EDX analysis plot. It
is shown that the composition near to the core of the
nanosphere (between 160 and 380 nm of distance) has a
higher content of Fe and O as compared to the outer
layer of the nanosphere, where C and Si contents are
higher. This fact testifies that the nanosphere composition is mainly Fe and O.
Discussion
The removal of the topmost layer of the CNT array and
the creation of a cavity upon the FSL irradiation are
Labunov et al. Nanoscale Research Letters 2013, 8:375
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1
2
Figure 2 Surface morphology of the FSL irradiated area of the CNT array (SEM). (1) Nanospheres located at the tips of the CNT bundles.
(2) Nanospheres located on top of CNT array (outside of the cavity). Inset: the entire 200 × 200 μm2 laser-processed surface.
a
2
1
3
b
c
Figure 3 SEM images of the nanospheres and their quantitative size distribution. (a) An image of the nanospheres (SEM). (1) A nanosphere
without a shell. (2) A nanosphere with the attached CNTs (might be covered with a shell), and (3) the nanospheres beading the CNT bundles.
(b) Representative grouping of the nanospheres. (c) Corresponding size distribution.
Labunov et al. Nanoscale Research Letters 2013, 8:375
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a
Page 6 of 10
c
b
1
3
1
3
2
2
45 nm
175 nm
100 nm
Figure 4 TEM images of the nanospheres in contact with CNTs in the irradiated area. (a) Nanospheres of larger diameter with (1) and
without (2) shells found at the tip of the thinned CNTs, and (3) nanospheres of smaller diameter beading CNTs. (b) Enlarged view of the
nanosphere encapsulated into the shell (1) containing some inclusions (2) and CNTs (3). (c) The nanospheres without shells.
achieved by means of ablation. The ultrashort pulse ablation process includes the absorption of optical radiation by bound and free electrons of the material, energy
transfer to the lattice, bond breaking, followed by evaporation of the material in a form of atoms or ions, and
vapor expansion into an ambient gas. Usually, weak
a
plasma is formed over the irradiated surface. The sputtered particles, upon losing energy, aggregate into clusters of different sizes, charges, and kinetic energies.
These resulting clusters can be either carried away from
the reaction zone or re-deposited back onto the target
(substrate) surface. This process is known as laser
b
200 nm
c
d
keV
Figure 5 EDX spectroscopy data on the composition of the FSL-irradiated CNT array on Si substrate. (a) EDX image of the investigated
area. (b, c) Element distribution along the diameter of the nanosphere. (d) EDX spectrum.
Labunov et al. Nanoscale Research Letters 2013, 8:375
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Page 7 of 10
Figure 6 Schematic of the proposed mechanism of the interaction of the FSL irradiation with CNT arrays.
machining; however, no adequate mechanism for the latter has been proposed.
Here, we propose a basic scheme of formation of the
cavity with the observed nanostructures as a result of
the interaction of FSL irradiation with the arrays of the
vertically aligned CNTs intercalated with Fe phase catalyst nanoparticles. Figure 6 shows the schematic of the
proposed mechanism.
In our case, the CNT array represents the target for
ablation that consists of two materials, i.e., graphitic
CNT walls and various iron phase intercalated within
the CNT channels and walls (Figure 6 (1)). Once the ablation threshold is reached, the topmost layer starts to
ablate away, i.e., both CNTs and the Fe phase nanoparticles. The ablation of the two materials (C and Fe)
occurs since the energy density even of a single pulse
(0.48 J/cm2) exceeded both of the reported ablation
thresholds of various carbonaceous materials (multiwall
CNTs, 0.046 J/cm2 [39]; single wall CNTs, 0.05 J/cm2
[40,41]; graphite, 0.13 J/cm2 [42]; graphene, 0.20 J/cm2
[43]); and the ablation threshold of iron, 0.18 to
0.19 J/cm2 [44,45]. The gradual ablation of the CNT
array leads to the formation of the cavity of approximately
10 μm depth. This ablation process of the C-Fe target is
rather complicated since two distinct materials are being
subjected simultaneously to multiple ultrashort laser
pulses during 3D scanning. It was found that the mechanism of solid ablation by the intense FSL irradiation is essentially the same [46]. Usually, at atmospheric pressure,
the ablation process occurring near to the threshold is always initiated by the ultrafast melting (bonds breaking) of
the material, which applies for iron. However, as it was
shown by Jeschke's group [47], graphite has the unique
property of exhibiting two distinct laser-induced
structural instabilities. At high absorption energies regime (>3.3 eV/atom), nonequilibrium melting occurs
that is followed by a fast evaporation. For low intensities,
slightly above the damage threshold (>2.0 eV/atom), ablation occurs via removal of intact graphite sheets. Taking
into account that the energy density of a single pulse
equals to F1 = 0.48 J/cm2, we calculated the absorbed energy per atom E0 using the equation [48]:
F1 ¼
eE 0 na d
;
1−R−T
ð1Þ
where e is the Coulomb constant, na is the atomic density,
d is the penetration depth of the light, R = 0.3 is the reflectivity, and T = 0 is the transmission of the material
which were assumed to be as for graphite [48]. The penetration depth was calculated using the Drude formula d =
λ/4πk with the wavelength of 790 nm and extinction coefficient k = 1.5 as for graphite [42]. It has been estimated
that the atomic density of our CNT arrays is approximately na = 7.52 × 1021 atoms/cm3 which is lower than
that of the graphite (na = 1.76 × 1023 atoms/cm3). The calculated value of the absorbed energy per atom even for a
single pulse, E0 = 66.95 eV/atom, is much higher than
those mentioned in [47] which implies that CNTs in these
conditions are burnt instantly.
As a result of C and Fe ablation, localized weak plasma
is formed over the irradiated surface (Figure 6 (2)). Both
substances exist in their plasma state for a short period
of time, while Fe undergoes a rapid condensation and
aggregates into spherical clusters (thermodynamically
the most favorable shape).
The energy density of the FSL beam, as it is shown in
Figure 6, reduces along the depth of CNT array in the
Labunov et al. Nanoscale Research Letters 2013, 8:375
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process of their interaction. At a certain depth (labeled
as ‘II’), the energy is not sufficient for the CNT covalent
bonds breaking and complete CNTs ablation. Only some
of the external walls of the multiwall CNTs are ablated,
and this leads to the thinning of the CNTs. The bundling
of thinned CNTs into the cones can mainly be caused by
the Van der Waals force or/and the magnetic interaction
of Fe phase nanoparticles. The Fe phase inclusions located in between the CNT walls most probably have not
undergone the complete evaporation but have been subject to a quick melting and resolidification; this led to
the formation of smaller nanospheres beading the conical shape of CNT bundles (Figure 6 (3)).
Noteworthy that the Fe phase transformations occur in
the presence of carbon atoms and though conditions are
quite similar to the floating CVD method, one can suppose that Fe particles can serve as a catalyst for the formation, during the cooling process, of graphitic architectures
(shells), covering the iron phase nanospheres. The shells
sometime contain CNTs, (Figure 4a,b, Figure 6 (4)). Besides, it was reported that multiwall CNTs and onions had
been obtained from graphite in vacuum at 7.5 J/cm2 FSL
fluence with the estimated growth time of 1 to 2 ns [49].
Similar to the case of CNTs synthesis process, due to the
stochastic process, not all of the catalyst particles facilitate
the growth of graphitic shells.
The iron phase nanospheres (with and without shells),
after their creation during the first FSL scans, freeze and
deposit on the surface of the irradiated area, while some
of them are sited slightly away (Figure 2).
During 3D scanning, the Fe-phase nanoparticles that
are sited nearer to the tip of the CNTs (labeled as ‘I’ in
Figure 6) would undergo the evaporation process each
scan, cluster and re-deposit back mostly on the tips of
the CNT conic bundles (Figure 1).
The gradual step-by-step ablation leads to coalescence
and increase in the diameter of the nanoparticles formed
during the first FSL scans. At a certain diameter of
nanospheres, due to Gaussian distribution of laser intensity, the incident energy might be not enough to evaporate the nanospheres completely and they undergo
melting instead. Being in a liquid state, they wet the surrounding CNTs. Once the FSL irradiation is stopped,
they freeze together forming the observed Fe phase
nanosphere/conical CNT bundle nanostructures (Fe/CNT
nanostructures), while the graphitic shells (if any) of a very
complicated structure (Figure 3a) are being extruded
during their cooling (Figure 6 (4)).
This scenario of the Fe/CNT nanostructure shape formation is the most realistic because it clearly explains
why in most cases Fe nanospheres are located directly
on the tips of the CNT cones. It is worth mentioning,
however, that at the beginning, the electrostatic forces
between CNTs are responsible for the formation of the
Page 8 of 10
CNT cones structure because sometimes the nanospheres
are too small to be able to link the nearby CNTs just by
wetting, which was observed in other works also [25].
The described mechanism is the most realistic due to
another reason since there is no clear periodicity of the
shape of the Fe/CNT nanostructures like, for example,
in the case of ‘black silicon’ where the cone formation is
governed by the initial ripple creation with the wavelength close to the central wavelength of the incident
laser [7].
Conclusions
In the present work, we investigated for the first time
the interaction of FSL irradiation with the arrays of vertically aligned carbon nanotubes intercalated with the
ferromagnetic (Fe phase) nanoparticles. The presence of
metal nanoparticles in CNT array plays the main role in
the energy absorption by the array. As a result of such
interaction, a novel composite nanostructured material
was obtained. This nanomaterial consists of tiny Fe
phase nanospheres attached to the tips of the CNT bundles of conical shape. We designated this material as Fe
phase nanosphere/conical CNT bundle nanostructures.
The mechanism of such nanostructure formation was
proposed. The importance of the present investigation is
defined by the possible applications of the obtained
results. The arrays of CNTs with the intercalated ferromagnetic nanoparticles, i.e., MFCNTs, may be considered
as an ideal medium for different magnetic applications.
The FSL irradiation may become an instrument for the
machining of the mentioned devices based on the arrays
of MFCNTs. Moreover, one could expect that the
obtained nanostructures would possess new optical properties which would find applications in photovoltaics and
plasmonics.
Abbreviations
CNT: Carbon nanotube; CVD: Chemical vapor deposition; EDX
spectroscopy: Energy-dispersive X-ray spectroscopy; Fe/CNT
nanostructures: Fe phase nanosphere/conical CNT bundle nanostructures;
FSL: Femtosecond laser; SEM: Scanning electron microscopy;
TEM: Transmission electron microscopy; XRD: X-ray diffraction.
Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
VL coordinated the study, analyzed the data, and contributed to the
manuscript preparation. AP synthesized the CNT arrays, performed structural
analyses of the samples, analyzed the experimental results, and contributed
to the manuscript preparation. SB carried out the femtosecond laser
irradiation of the CNT arrays and analyzed the data. SF performed EDX study
of the irradiated CNTs. BS and BKT analyzed the data and contributed to the
manuscript preparation. YS and AB carried out TEM and analyzed the data.
All authors read and approved the final manuscript.
Acknowledgements
We thank the Head of the Government Center ‘BelMicroAnalysis’
(scientific and technical center ‘Belmicrosystems’) V. Pilipenko for the access
to SEM facilities (Hitachi S-4800 FE-SEM). We are grateful to J. Fedotova and
Labunov et al. Nanoscale Research Letters 2013, 8:375
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K. Yanushkevich for providing Mössbauer spectroscopy and XRD diffraction
measurements of CNT arrays, correspondingly.
Author details
1
Laboratory of Integrated Micro- and Nanosystems, Belarusian State
University of Informatics and Radioelectronics, P. Brovka St. 6, Minsk 220013,
Republic of Belarus. 2Laboratory of Optical Diagnostics, B.I. Stepanov Institute
of Physics of the National Academy of Sciences of Belarus, Minsk 220072,
Republic of Belarus. 3Laboratory of Hydrogen Energy, Institute of Heat and
Mass Transfer of the National Academy of Sciences of Belarus, Minsk 220072,
Belarus. 4School of Electrical and Electronic Engineering, Nanyang
Technological University, Singapore 639798, Singapore.
5
Scientific-Manufacturing Complex Technological Centre MIET, K-498,
Moscow 103498, Russia.
Received: 28 June 2013 Accepted: 22 August 2013
Published: 3 September 2013
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doi:10.1186/1556-276X-8-375
Cite this article as: Labunov et al.: Femtosecond laser modification of an
array of vertically aligned carbon nanotubes intercalated with Fe phase
nanoparticles. Nanoscale Research Letters 2013 8:375.
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